Open Access Article
Yu Liu
a,
Chunyan Liu
a,
Zhihui Dai
abc and
Weiliang Guo
*ab
aCollaborative Innovation Center of Biomedical Functional Materials, School of Chemistry and Materials Science, Nanjing Normal University, Nanjing 210023, China. E-mail: guowl@njnu.edu.cn
bState Key Laboratory of Analytical Chemistry for Life Science, Nanjing University, Nanjing 210023, China
cSchool of Chemistry and Molecular Engineering, Nanjing Tech University, Nanjing 211816, China
First published on 16th March 2026
Electrochemiluminescence (ECL) immunoassays have emerged as a powerful method for multiplex biomarker detection due to their advantages of low background noise, high sensitivity, and ease of miniaturization, holding significant applications in precision medicine and in vitro diagnostics (IVD). This article systematically reviews recent advances in ECL-based multiplex immunoassays, focusing on two primary strategies for achieving multiplex detection. One is the spectrum-resolved strategy that enables differentiation of multiple targets by utilizing multicolor ECL luminophores, such as metal complexes and quantum dots, which emit light at distinct wavelengths. The other is the spatially resolved strategy that employs technologies including microarrays, microfluidic chips, and encoded microbeads to physically separate detection sites, allowing high-throughput analysis with just one luminophore. This review summarizes innovative designs under both strategies aimed at enhancing detection performance, discusses their applications in the diagnosis of diseases such as cancer and cardiovascular disorders, and addresses current challenges related to analytical performance, system integration, and clinical use. Finally, prospects for ECL technology in IVD and precision medicine are outlined.
In recent years, numerous efforts have focused on developing novel multiplex immunoassays by integrating techniques such as radioisotopic,8 optical,9–11 spectroscopic,12 and electrochemical methods.13 Electrochemiluminescence (ECL) refers to a light-emitting process in which the excited-state species is generated via high energy electron transfer reactions at the electrode surface.14–16 In comparison with the methods that rely on external light excitation such as fluorescence and surface plasmon resonance, ECL reactions do not require an external light source for excitation, thus avoiding interference from light scattering and offering outstanding advantages of high detection sensitivity and near-zero background.17 When compared with chemiluminescence that takes place in a mixed solution, ECL reactions occur near the electrode surface and are highly sensitive to interfacial processes, exhibiting excellent spatiotemporal control.18
A wide variety of ECL luminophores, ranging from aromatic hydrocarbons and metal complexes to nanomaterials, have been synthesized.19–21 However, tris(2,2′-bipyridyl)ruthenium(II) (Ru(bpy)32+) remains the most extensively employed in fundamental studies. In the presence of tri-n-propylamine (TPrA) as a co-reactant, Ru(bpy)32+ exhibits high and stable ECL emission in aqueous solutions, thus making ECL one of the most powerful commercial analytical techniques.14,22 For instance, over 100 distinct biomarkers (e.g., cancer, inflammatory, or cardiac biomarkers, as well as hormones) can be determined based on ECL immunoassay devices commercialized by Roche Diagnostics and Meso Scale Discovery (MSD).
This review offers a comprehensive overview of ECL immunoassays, designed specifically for researchers new to the field. We begin with a brief introduction to the fundamental principles of ECL, followed by a summary of recent progress in both spectrally and spatially resolved strategies for constructing multiplexed ECL immunoassays. Key achievements in enhancing analytical performance are also highlighted. Finally, we discuss the current challenges and future perspectives for the advancement of ECL immunoassays.
In general, the annihilation mechanism can be summarized as follows. The potential of the working electrode is switched rapidly between two values. At the cathode, luminophore A is reduced to A˙− (eqn (1)), while at the anode, luminophore D is oxidized to D˙+ (eqn (2)). These two species annihilate near the electrode surface to generate the excited-state species A* (eqn (3)), which then emits light (eqn (4)). Depending on the identity of the reactants, the process is classified as “homogeneous annihilation” (A and D are the same species) or “heterogeneous annihilation” (A and D are different species).25,26 For example, in the homogeneous annihilation of Ru(bpy)32+, oxidized Ru(bpy)33+ and reduced Ru(bpy)3+ react to produce the excited state Ru(bpy)32+* with concomitant light emission. A representative heterogeneous annihilation process is the cross-reaction between the DPA anion radical and the N,N,N′,N′-tetramethyl-p-phenylenediamine (TMPD) cation radical.27
| A + e− → A˙− (reduction at the electrode) | (1) |
| D → D˙+ + e− (oxidation at the electrode) | (2) |
| D˙+ + A˙− → D + A* (excited state formation) | (3) |
| A* → A + hv (light emission) | (4) |
Depending on the relationship between the reaction enthalpy change and the excited state energy (eqn (5)), where −ΔHann is the enthalpy of ion annihilation and EP is the peak potential for electrochemical oxidation or reduction, the annihilation pathway can be further classified into the singlet-state route (S-route) and the triplet-state route (T-route).28
| −ΔHann = Ep(D˙+/D) − Ep(A/A˙−) − 0.157 | (5) |
| S-route: D˙+ + A˙− → D + 1A* (excited singlet formation) | (6) |
When −ΔHann < ES, the system is energy-deficient and follows the T-route. Here, the triplet excited state 3A* is initially formed (eqn (7)), followed by its conversion to 1A* via triplet–triplet annihilation (eqn (8)), as exemplified by the TMPD˙+/DPA˙− system.31
| T‐route: D˙+ + A˙− → D + 3A* (excited triplet formation) | (7) |
| 3A* + 3A* → A + 1A* (triplet–triplet annihilation) | (8) |
Oxidative–reductive co-reactants generate strong reducing intermediates upon electrochemical oxidation, which then reduce the oxidized luminophore to form the excited state. This type of co-reactant is the most widely used, with typical examples including oxalate ions (C2O42−) and TPrA. Oxalate, the first discovered co-reactant, undergoes bond cleavage under anodic oxidation conditions to produce the strongly reducing CO2˙− (eqn (9)). Simultaneously, the luminophore Ru(bpy)32+ is oxidized to Ru(bpy)33+ (eqn (10)). Subsequently, CO2˙− reduces Ru(bpy)33+ to the excited state Ru(bpy)32+* (eqn (11)), which then emits light (eqn (12)).22
| C2O42− − e− → [C2O4˙−] → CO2˙− + CO2 | (9) |
| Ru(bpy)32+ → Ru(bpy)33+ + e− | (10) |
| CO2˙− + Ru(bpy)33+ → Ru(bpy)32+* + CO2 | (11) |
| Ru(bpy)32+* → Ru(bpy)32+ + hv | (12) |
TPrA, as a co-reactant in commercial ECL systems, exhibits a more complex oxidation process involving multiple parallel reaction pathways.33,34 Initially, TPrA undergoes electrochemical oxidation at the electrode surface to form the radical cation TPrA˙+ (eqn (13)), which rapidly undergoes deprotonation to yield the strongly reducing intermediate TPrA˙ (eqn (14)).35
| TPrA → TPrA˙+ + e− | (13) |
| TPrA˙+ → TPrA˙ + H+ | (14) |
Fig. 1 summarizes several proposed reaction mechanisms. For instance, this reducing intermediate can directly reduce Ru(bpy)33+ to generate the excited state (Fig. 1a). Simultaneously, TPrA˙ can also reduce Ru(bpy)32+ to Ru(bpy)3+, which subsequently undergoes an annihilation reaction with Ru(bpy)33+ to produce light emission (Fig. 1b). Fig. 1c illustrates the generation of the excited state Ru(bpy)32+* via the so-called low oxidation potential pathway, where only TPrA, but not Ru(bpy)32+, undergoes electrochemical oxidation. In contrast, in the catalytic pathway TPrA˙+ and TPrA˙ are generated via homogeneous oxidation between electrogenerated Ru(bpy)33+ and TPrA, rather than through direct electrochemical oxidation of TPrA at the electrode surface (Fig. 1d). Notably, this pathway is favored when the concentration of Ru(bpy)32+ is high.36
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| Fig. 1 (a)–(d) Proposed mechanism for Ru(bpy)32+/TPrA ECL excited state formation and light emission. | ||
Reductive–oxidative co-reactants generate strong oxidizing intermediates upon electrochemical reduction, which then oxidize the reduced luminophore to yield the excited state. A typical example is peroxydisulfate (S2O82−), which undergoes cathodic reduction to generate SO4˙− (eqn (15)), possessing an extremely high oxidation potential (3.15 V vs. SCE). Ru(bpy)32+ is first reduced to Ru(bpy)3+ (eqn (16)) and is subsequently oxidized by SO4˙− to the emissive excited state (eqn (17)).37
| S2O82− + e− → SO4˙− + SO42− | (15) |
| Ru(bpy)32+ + e− → Ru(bpy)3+ | (16) |
| Ru(bpy)3+ + SO4˙− → Ru(bpy)32+* + SO42− | (17) |
At present, a deeper understanding of ECL mechanisms is achieved, facilitated by various advanced techniques including optical microscopy, mass spectrometry, and spectroscopic measurement. For example, electrochemistry coupled mass spectrometry (ECMS) enables the capture and identification of short-lived intermediates (e.g., radical cation TPrA˙+ and neutral radical TPrA˙) involved in ECL reactions, providing direct evidence for co-reactant pathways and transforming previously proposed ECL mechanisms into experimentally validated findings.38,39 Furthermore, both ECL-based microscopy (ECLM) and ECL self-interference spectroscopy (ECLIS) allow the observation of the spatial distribution of the ECL-emitting layer, and have been employed to decipher ECL reaction mechanisms. By measuring the thickness of the emission layer, the switch of the dominant ECL pathway can be resolved and regulated via the luminophore concentration or the concentration ratio of the luminophore to the co-reactant.40–42
In spectrum-resolved multiplex ECL immunoassays, the spectral characteristics of the luminophores directly determine the number of targets that can be simultaneously detected. However, the major limitation of molecular luminophores is their broad full-width at half-maximum, which results in substantial spectral overlap and constrains the multiplexing capacity of spectrum-resolved ECL immunoassays. Su et al. developed a potential-modulated spectrum-resolved strategy based on novel ruthenium(II) and iridium(III) complexes, thus constructing a dual-resolved ECL system for multiplex immunoassays (Fig. 2a). They synthesized Ru(bpy)2(dvbpy)2+ (bpy = 2,2′-bipyridine; dvbpy = 4,4′-bis(4-vinylphenyl)-2,2′-bipyridine, λmax = 636 nm) and Ir(dFCF3ppy)2(dtbbpy)+ (dFCF3ppy = 3,5-difluoro-2-[5-(trifluoromethyl)-2-pyridinyl]-phenyl; dtbbpy = 4,4′-bis(tert-butyl)-2,2′-bipyridine, λmax = 491 nm), achieving a 145 nm spectral separation, and further realized potential-regulated switch on/off emission of Ir(ppy)3 (λmax = 526 nm), thus allowing for the potential-resolved ECL emission. As illustrated in Fig. 2b, applying sequential potentials at +0.74 V, +1.33 V, and +1.75 V selectively activated each luminophore, enabling both spectral and potential resolution. Building on this principle, these three luminophores were loaded into polystyrene beads to encode detection antibodies for carcinoembryonic antigen (CEA), alpha-fetoprotein (AFP), and beta-human chorionic gonadotropin (β-hCG). This ultimately enabled the simultaneous identification of all three cancer markers in a single sample and scan.45
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| Fig. 2 Potential-resolved and spectrum-resolved ECL strategy for multiplex immunoassays. (a) Schematic procedure for the simultaneous detection of three tumor markers. (b) ECL detection platform and the principle of selectively activating three luminophores at different applied potentials. Reprinted with permission from ref. 45. Copyright 2018 American Chemical Society. | ||
Quantum dots (QDs) demonstrate the theoretical capability for simultaneous discrimination of four to five or even more targets, owing to their extremely narrow emission peaks, tunable wavelengths, and co-excitation capacity. As one of the earliest labeling materials applied in spectrum-resolved ECL immunoassays, QDs exhibit emission spectra covering the visible, near-infrared, and even far-infrared regions.46 This excellent spectral tunability provides a crucial material foundation for the development of ECL-based multiplex detection strategies. Miao et al. developed dual-stabilizer-capped CdSe (λmax = 550 nm) and CdTe (λmax = 776 nm) nanocrystals as ECL labels for the simultaneous detection of AFP and CEA, with the limit of detection (LOD) of 10 fg mL−1 and 1 pg mL−1, respectively. Using ammonium persulfate ((NH4)2S2O8) as a cathodic ECL co-reactant, the ECL signal was generated during cathodic potential scanning. The resulting ECL spectra from the two immobilized luminophores effectively eliminated cross-talk, thereby overcoming the spectral overlap inherent in traditional multiplex ECL assays.47
Furthermore, Zou et al. reported a spectrally resolved three-color ECL multiplex immunoassay. Firstly, they synthesized dual-stabilizer-capped CdSe (λmax = 550 nm), CdTe (λmax = 650 nm), and CdTe (λmax = 776 nm) nanocrystals. By applying a potential in a buffer containing (NH4)2S2O8 and collecting emission intensities across wavelengths via a spectrometer, they successfully achieved simultaneous detection of three tumor markers, namely CEA, prostate-specific antigen (PSA), and AFP, on a single electrode interface, with LODs of 1, 10, and 0.01 pg mL−1, respectively. With the ongoing development of new monochromatic ECL luminophores covering broader spectral ranges, this strategy could potentially be extended to detect four or more targets simultaneously.48
To fundamentally solve the problems of low efficiency and poor stability of conventional QDs, innovative core/shell/shell structures (CdSe core–CdS intermediate layer–ZnS outer layer) were developed by Su and coworkers. These QDs maintained near-unity photoluminescence quantum yields (>90%) and narrow emission peaks in aqueous solution. Their ECL efficiency was enhanced by six orders of magnitude compared to the conventional Ru(bpy)32+ emitter, and the relative standard deviation of the luminescence intensity remained below 1% over 125 consecutive potential scan cycles, demonstrating excellent operational stability. They precisely controlled the CdSe core size to prepare three-color quantum dots emitting at 549 nm (green), 592 nm (yellow), and 643 nm (red), with emission wavelength intervals of approximately 50 nm (Fig. 3a). As illustrated in Fig. 3b, by mixing these luminophores in a phosphate-buffered solution containing K2S2O8 and applying a cathodic potential sweep (−0.9 V to −1.3 V) on a single working electrode, the ECL emissions of the different QDs could be sequentially and selectively excited. The resulting signals were spectrally well-resolved with negligible crosstalk (Fig. 3c–e), providing a practical strategy for high-throughput detection of multiple biomarkers.49
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| Fig. 3 (a) Normalized PL spectra and ECL photographs of green-, yellow-, and red-emitting CdSe/CdS/ZnS core/shell/shell QDs. (b) ECL-potential spectra of a mixed solution containing the three colors of QDs. (c–e) ECL spectra and corresponding photographs (insets) of the three-component mixed system at three different applied potentials. Reprinted with permission from ref. 49. Copyright 2020 American Chemical Society. | ||
Due to the restricted spectral range of the visible region (400–750 nm), spectral multiplexing is constrained by the limited number of resolvable channels. The development of near-infrared (NIR) luminophores can extend the detectable spectral window, thereby increasing the number of resolvable channels for multiplex detection. Moreover, NIR luminophores offer minimal autofluorescence, significantly reducing background noise and thus enhancing the signal-to-noise ratio compared to conventional UV-visible detection. However, most aqueous NIR ECL luminophores, such as graphene oxide and CdTe QDs, typically emit below 800 nm and suffer from substantial spectral overlap in multiplexed detection, compromising both sensitivity and accuracy. To address this issue, Shen et al. reported the fabrication of an innovative NIR ECL luminophore based on bovine serum albumin-stabilized silver nanoclusters (BSA-Ag NCs). When coupled with TiO2 nanoparticles as a co-reactant accelerator, the luminophore enabled highly efficient anodic ECL emission at 904 nm in aqueous medium to surpass the 900 nm threshold. By tagging anti-cancer antigen 125 (anti-CA125), anti-carbohydrate antigen 19-9 (anti-CA19-9) and anti-cardiac troponin I (anti-cTnI) secondary antibodies with CdSe NCs (λmax = 553 nm), CdTe NCs (λmax = 676 nm) and the new BSA-Ag NCs (λmax = 904 nm), respectively, they achieved three baseline-resolved emission peaks in a single potential sweep, thus demonstrating a three-color, spectrally resolved ECL multiplex immunoassay on a single electrode surface (Fig. 4a).50
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| Fig. 4 (a) Spectrum-resolved ECL MIA toward samples containing CA125, CA19-9 and cTnI at different concentrations. Adapted with permission from ref. 50. Copyright 2020 Elsevier B.V. (b) Schematic illustration of the potential- and spectrum-resolved dual-mode ECL measurement process for the simultaneous detection of AFP, CA125, and CA19-9. Adapted with permission from ref. 52. Copyright 2024 Elsevier B.V. | ||
Spectrum-resolved measurement using spectrometers often suffers from sensitivity loss due to the slits in the monochromator. Photomultiplier tubes (PMTs), by contrast, provide highly sensitive detection and enable spectral resolution without a sensitivity trade-off, when combined with optical filters. Zou et al. achieved spectrally resolved multiplexed ECL detection by combining two PMTs with a dichroic mirror. ECL emissions from two QDs, namely, CdSe (550 nm) and CdTe (790 nm), were completely separated by the dichroic mirror and measured by the two PMTs, respectively. As a result, this dual-band ECL detection platform exhibited LODs of 1 pg mL−1 for AFP and 1 mU mL−1 for CA125, avoiding spectral overlap and improving detection sensitivity.51 Very recently, Shen et al. reported a potential and spectrum dual-resolved ECL immunoassay based on a custom three-channel bandpass filter wheel (Fig. 4b). In a single cathodic sweep, perylene tetracarboxylic acid@carboxylic carbon nanotubes (710 nm) were first activated at lower potentials (0–0.8 V) for AFP detection. After rotating the filter wheel, CdSe (550 nm) and CdTe (750 nm) quantum dots were sequentially read out for spectrum-resolved detection of CA125 and CA19-9. The assay achieved detection limits of 0.53 fg mL−1, 0.058 mU mL−1, and 0.11 mU mL−1 for AFP, CA125, and CA19-9, respectively, which matched well with the performance of single-plex immunoassays. This platform eliminates the need for spectrometers and offers low-cost and high-throughput ECL detection.52
In addition to the metal complexes and quantum dots discussed above, a variety of other materials have been synthesized for spectrum-resolved ECL immunoassays. For instance, metal-free carbon-based nanomaterials have attracted considerable attention due to their good biocompatibility and tunable photoelectric properties.53 Table 1 summarizes the recent advances in spectrum-resolved multiplex ECL immunoassays employing various luminophores. The analytical performances of these assays, including the limit of detection and linear ranges, are also compared.
| No. | ECL luminophores & λem max | Targets | Limit of detection | Linear range | Ref. |
|---|---|---|---|---|---|
| 1 | CdSe QDs; 550 nm | AFP | 10 fg mL−1 | 50–1.0 × 105 fg mL−1 | 47 |
| CdTe QDs; 776 nm | CEA | 1 pg mL−1 | 10–1.0 × 104 pg mL−1 | ||
| 2 | CdSe QDs; 550 nm | CEA | 1.0 pg mL−1 | 0.01–10 ng mL−1 | 48 |
| CdTe QDs; 650 nm | PSA | 10.0 pg mL−1 | 0.1–100 ng mL−1 | ||
| CdTe QDs; 776 nm | AFP | 0.01 pg mL−1 | 0.1–100 pg mL−1 | ||
| 3 | CdSe QDs; 553 nm | CA125 | 0.035 mU mL−1 | 0.1–1.0 × 103 mU mL−1 | 50 |
| CdTe QDs; 676 nm | CA19-9 | 0.087 mU mL−1 | 0.3–1.0 × 103 mU mL−1 | ||
| BSA-Ag NCs; 904 nm | cTnI | 0.016 pg mL−1 | 0.03–100 pg mL−1 | ||
| 4 | CdSe QDs; 550 nm | AFP | 1 pg mL−1 | 5–5.0 × 103 pg mL−1 | 51 |
| CdTe QDs; 790 nm | CA125 | 1 mU mL−1 | 5–1.0 × 103 mU mL−1 | ||
| 5 | CdSe QDs; 550 nm | CA125 | 0.058 mU mL−1 | 0.1–300 mU mL−1 | 52 |
| CdTe QDs; 750 nm | CA19-9 | 0.11 mU mL−1 | 0.3–300 mU mL−1 | ||
| PTCA@CNTs; 710 nm | AFP | 0.53 fg mL−1 | 0.003–10 pg mL−1 | ||
| 6 | CNNs; 438 nm | CA19-9 | 0.083 U mL−1 | 0.01–80 U mL−1 | 53 |
| S-CNNS; 510 nm | Mesothelin | 0.91 ng mL−1 | 0.001–50 μg mL−1 | ||
| 7 | Zn-AIE-AuNCs; 485 nm | CEA | 0.3 pg mL−1 | 1.0–5 × 104 pg mL−1 | 54 |
| CIS@ZnS nanocrystals; 775 nm | P53 | 0.5 pM | 1.0–5 × 104 pM |
Microarrays are commonly used substrates for immobilizing different capture antibodies at defined locations, thus achieving spatial separation of detection sites. A typical example is the work reported by Pfeifer et al., who constructed 50 spatially separated detection spots on a 4 mm diameter electrode (Fig. 5a–c), allowing for the simultaneous determination of two triplex biomarker panels for traumatic brain injury and cardiac diseases, and achieving detection limits of 1–33 pg mL−1 with good reproducibility and specificity (cross-reactivity <6%).57 In addition, a triple ECL detection array was constructed by the combined use of disposable screen-printed carbon electrodes and a portable ECL reader, which enables the simultaneous detection of three biomarkers, namely GFAP, h-FABP, and S100β, without cross-reactivity. In comparison with conventional imaging techniques such as CT and MRI, this approach offers advantages including simple operation, fast detection, and low cost, making it particularly suitable for resource-limited environments such as accident sites and remote areas.58
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| Fig. 5 (a) Schematic illustration of the disposable microfluidic cartridge and fluidic channel design. (b) Photograph of the cartridge held in hand. (c) Photograph of the cartridge loaded into the drawer of the ECL reader prior to measurement. Reprinted with permission from ref. 57. Copyright 2022 American Association for the Advancement of Science. (d) Electrode layout with an eight-channel circular array, a common cathode, a signal chamber, and an assay chamber. (e) Chip assembly: plastic fluidic layer bonded to a PCB, integrated magnet array, and pogo pins for electrical connection. (f) Signal detection: applied potential drives the ECL reaction in the signal chamber for real-time imaging using a CCD camera. Reprinted with permission from ref. 61. Copyright 2022 American Association for the Advancement of Science. | ||
The aforementioned studies usually employed nano-spotting or 3D printing to precisely immobilize or spatially separate capture antibodies on the substrate electrode. Alternatively, Cui et al. reported a different approach based on a single-electrode configuration for microarray fabrication, achieving simultaneous quantitative detection of acute myocardial infarction (AMI) biomarkers, such as cTnI, h-FABP, and copeptin. Validation with 260 clinical serum samples demonstrated 100% sensitivity and specificity, significantly surpassing the conventional high-sensitivity cardiac troponin T (hs-cTnT) assay, and reducing the misdiagnosis rate by over 20% within the critical 3–12 hour window after symptom onset. It thus provides a reliable measurement tool for the early and accurate diagnosis of AMI.59
Furthermore, microfluidic chips enable automated sample and reagent delivery, making them a popular platform for multiplexed ECL immunoassays. Rusling and coworkers fabricated a monolithic 3D-printed microfluidic chip integrated with an automated micro-pump controller. The assay can complete the simultaneous detection of eight prostate cancer biomarkers in human serum in only 25 minutes, with detection limits as low as 78–110 fg mL−1, providing a powerful tool for rapid clinical multi-parameter diagnosis.60 As illustrated in Fig. 5d–f, a novel sensing system termed the ECLipse (ECL in paired signal electrode) chip was constructed, in which the biorecognition and ECL generation processes were physically separated via bipolar electrodes (BPEs). In this modular design, the triangular tips of eight BPEs were positioned within a single signal chamber containing ECL luminophores, while biorecognition reactions occurred in eight independent assay chambers, thus allowing for the simultaneous detection of eight targets in a single run. Meanwhile, this chip achieved detection limits of 15–230 fg mL−1 and an over 7000-fold increase in detection sensitivity compared to conventional ELISA.61
In contrast to planar microarrays or microfluidic chips that rely on precisely patterned electrodes or physically isolated channels to achieve spatial resolution, spot-free microbead-based arrays offer a fundamentally different and highly versatile approach for multiplexed ECL immunoassays. Rather than immobilizing capture antibodies on predefined two-dimensional substrates, microbeads function as addressable carriers for antibody immobilization. By encoding microbeads with fluorescent dyes, shapes, or diameters, bead-based ECL immunoassays can achieve high-order multiplexing. As shown in Fig. 6a, Sojic and Walt demonstrated a bead-based microarray that combines fluorescence encoding with single-bead ECL imaging. Fluorescence encoding was achieved by doping beads with varying Eu3+ dye concentrations and conjugating them to specific capture antibodies, allowing each bead to be identified by its characteristic fluorescence intensity. After loading onto a gold-coated optical fiber bundle electrode microwell array, the encoded beads were subjected to a sandwich immunoassay using an ECL luminophore (SA–Ru complex), ultimately enabling spatially resolved ECL imaging at the single-bead level.62
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| Fig. 6 (a) Schematic of the bead-based multiplexed ECL immunoassay using a Ru(bpy)32+/TPrA system with spatial resolution. Reprinted with permission from ref. 62. Copyright 2009 American Chemical Society. (b) Comparison of ECL generation efficiency between GMBs and MMBs under different pathways. Reprinted with permission from ref. 63. Copyright 2023 American Chemical Society. | ||
As previously reported, the main limitation in conventional bead-based ECL immunoassays originates from the low oxidation potential pathway.40 Because the ECL-emitting region around the bead is determined by the diffusion distance of TPrA˙+, and its lifetime is only 0.2 ms, ECL generation is thus limited to a zone within 3 μm of the substrate electrode surface. To overcome this constraint, gold-coated microbeads (GMBs) were employed as conductive carriers and for constructing proximity ECL generation (Fig. 6b). As demonstrated, GMBs can function as spherical ultramicroelectrodes for direct co-reactant oxidation on their surface, thus shortening radical diffusion distances and enhancing ECL signals. When using CRP as a model analyte, the GMB-based ECL immunoassay achieved a 4.96-fold increase in ECL intensity and a 21.7-fold enhancement in turnover frequency over conventional magnetic microbeads, consequently improving the detection limit from 0.35 ng mL−1 to 0.12 ng mL−1. Moreover, because the ECL generation at GMBs is no longer restricted by the diffusion distance of TPrA˙+, the size-encoded multiplex immunoassay is eventually established for four AMI biomarkers, namely CRP, cTnI, FABP, and Myo.63
As discussed above, the spatially resolved strategy can be implemented using planar microarrays, microfluidic chips, or encoded bead-based microarrays. Table 2 summarizes representative spatially resolved multiplexed ECL immunoassays, detailing their spatial encoding principles, multiplexing capacity, key innovations, detection performance, and commercial availability. These platforms enable multiplexing ranging from dual-plex to eight-plex detection and exhibit a sensitivity improvement of several orders of magnitude over conventional ELISA, with detection limits reaching fg mL−1 levels.
| Technology platform | Multiplexing capacity | Key innovation | Detection performance | Commercial availability | Ref. |
|---|---|---|---|---|---|
| Spatially resolved ECL immunoassay | 3-Plex (2 panels of biomarkers) | Low-cost 3D-printed chip, physical isolation of detection zones | 1–33 pg mL−1, cross-reactivity < 6% | Partially available | 57 |
| Screen-printed electrode array | 3-Plex | Portable ECL reader suitable for POC settings | GFAP: 6.94 pg mL−1, h-FABP: 1.35 pg mL−1, S100β: 15.73 pg mL−1 | Fully available | 58 |
| Triplex diagnostic microchip | 3-Plex | Chemiluminescence immuno-gold nanoassemblies (ciGold) | 0.014–0.053 ng L−1, clinical validation showed 100% sensitivity | Partially available | 59 |
| 3D-printed microfluidic array | 8-Plex | Automated integration of 3D-printed microfluidic chip | 78–110 fg mL−1, completed in 25 minutes | Partially available | 60 |
| ECLipse platform | 8-Plex | Separation of biorecognition and signal generation regions using bipolar electrodes | 15–230 fg mL−1, sensitivity increased by 7000-fold | Partially available | 61 |
| Bead-based array | Multiplex (variable) | Single-bead-level ECL imaging, fluorescence encoding for bead identification | Single-molecule-level sensitivity | Fully available | 62 |
| Gold microbead-encoded platform | 4-Plex | Proximity ECL, spherical ultramicroelectrodes generating reactive radicals autonomously | CRP: 0.12 ng mL−1 | Fully available | 63 |
| Ultra-sensitive microfluidic immunoarray | 4-Plex | Streptavidin–poly-HRP signal amplification | 0.013–0.13 fg mL−1, dynamic range spanning five orders of magnitude | Partially available | 64 |
| CRISPR-ECL array | 3-Plex | Integration of the CRISPR/Cas13a system with a 3D-printed microfluidic array | Sub-fg mL−1 level sensitivity | Partially available | 65 |
| Spatial-potential resolved BPE-ECL system | 2-Plex | Non-precious metal electrocatalyst CuHCF for signal amplification | miRNA-122: 40 fM; CEA: 3 fg mL−1 | Fully available | 66 |
Thanks to the remarkable advantages of low background noise, high sensitivity, and high throughput, ECL immunoassays have emerged as a powerful method for multi-biomarker detection in vitro diagnostics and point-of-care testing. Despite significant progress in recent years, some challenges remain to be addressed. For example, although a variety of ECL luminophores have been synthesized, only Ru(bpy)32+ and its derivatives have found practical application. This limited selection severely restricts the clinical use of spectrum-resolved multiplexed immunoassays. In addition, although numerous innovative ECL assays based on spectrum- and/or spatially resolved strategies have been established at the methodological level, their validation using real samples containing complex matrices remains limited. Furthermore, standardized protocols for multiplexed ECL immunoassays are still lacking.
Future efforts should focus on improving the spatiotemporal resolution of ECL detection that offers a promising pathway to significantly improve analysis speed in multiplexed immunoassays. Nowadays, electron multiplying charge coupled devices (EMCCDs) enable high-speed and real-time imaging of ECL emissions from single entities, while achieving microsecond temporal resolution and spatial resolution down to tens of nanometers.67,68 However, the imaging time for ECL immunoassays typically ranges from seconds to minutes. Achieving rapid signal acquisition would substantially reduce total assay time, which is a critical improvement for time-sensitive applications such as emergency diagnostics and point-of-care testing.
On the other hand, the application of artificial intelligence to ECL imaging and spectral analysis offers new opportunities for improving detection accuracy. Machine learning algorithms can assist in identifying spatial features, discriminating signals from background noise, and resolving overlapping emission spectra from multiple luminophores, thereby enabling reliable quantification. The combination of high-speed spatiotemporal imaging with intelligent data processing is expected to advance multiplexed ECL immunoassays toward rapid point-of-care testing, higher throughput, improved sensitivity and specificity, and greater automation.
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